EbyE fluctuations in the EKRT pQCD+saturation ...crunch.ikp.physik.tu-darmstadt.de/erice/2016/sec/talks/thursday/... · EbyE fluctuations in the EKRT ... ultrarelativistic A+A collisions

EbyE fluctuations in the EKRT pQCD+saturation+hydrodynamics model:

Determining QCD matter shear viscosity in ultrarelativistic A+A collisions

Kari J. Eskola Department of Physics, University of Jyväskylä & Helsinki Institute of Physics

International School of Nuclear Physics, Erice 22.9.2016

Reviewing the results from: Phys.Rev. C93 (2016) 024907, arXiv:1505.02677 [hep-ph] Phys.Rev. C93 (2016) 014912, arXiv:1511.04296 [hep-ph]

In collaboration with Harri Niemi, J.W. Goethe University, Frankfurt Risto Paatelainen, University of Santiago de Compostela Kimmo Tuominen, University of Helsinki

Talk plan 1. Background and some history - original EKRT model 2. Recent developments in EKRT [Phys.Rev. C93 (2016) 024907] - NLO pQCD, EbyE viscous hydro framework - Comparison with LHC & RHIC data η/s(T) 3. Predictions for the 5.02 TeV Pb+Pb LHC run - Compare [Phys.Rev. C93 (2016) 014912] with measurements

η/s(T) = ? A Challenge!

1. Background: pQCD + saturation + hydro = EKRT model

RA

Collinear factorization + pQCD # few-GeV gluon ”minijets” in A+A, y at ΔY, pT≥ p0

Saturation of minijet (= gluon) production when p0 = 1…2 GeV: lower-pT gluons conjectured to be not relevant due to fusion of produced gluons

[ Concept of saturation introduced by Gribov,Levin&Ryskin ’83, Mueller&Qiu ’86, and in the CGC framework by McLerran&Venugopalan ’94, and noticed by us in ’96 ]

[KJE,Kajantie,Ruuskanen,Tuominen, hep-ph/9909456, NPB570 (2000) 379]

A

A minijets

N, ET

pT

Collision geometry

pQCD + nuclear PDFs

x

y

Saturation of gluon production in A+A at b=0 in ΔY=1 when

RA psat=p0(√s, A) minijet Ni(psat) and ET(psat)

• QGP forms early: τi=1/psat = 0.1 …0.2 fm • the produced QGP looks ”thermal” in ET/N : - may assume early thermalization, τ0= τi - initial conditions for ideal hydro (1 D BJ) Ni(psat) or ET(psat) S_i = S_f Nf

Hard scaling A4/3 was tamed to ~A & Power law in cms-energy !

[ Comment in 2001 in CERN (=after the first RHIC data) ”It can never be a power-law in s!” ] 4

• Predicted very definite scaling laws, before any(!) RHIC data

[Original EKRT model]

[EKRT, hep-ph/9909456, NPB570 (2000) 379]

[EKRT, hep-ph/9909456, NPB570 (2000) 379]

A more detailed EKRT-model prediction - ideal 1+1 D hydro, LO nPDFs + pQCD partly NLO [KJE, Tuominen, Phys.Rev. D63 (2001) 114006]

[KJE,Ruuskanen,Räsänen, Tuominen,NPA696:715,2001] - made before the 200 GeV RHIC data - dNch/dη = 1782 for 2.76 ATeV

EKRT

EKRT correct within ~7%

ALICE, PRL105:252301,2010 1584 +- 76

Our prediction 2560 for the max cms-energy was VERY LOW AT THE TIME, << 8000, but after RHIC 200 GeV data, suddenly WE were on the high-side of predictions! [Miklos in 2007 at CERN: ”I’m glad your knees don’t wobble!” (but they did…) ]

RHIC

LHC

5


Successful framework tests in Au+Au at RHIC (still with ideal hydro)

[KJE, Honkanen, Niemi, Ruuskanen, Räsänen, PRC72 (2005) 044904]

EKRT observation: To get these pT spectra right means a factor THREE(!) reduction from the computed ETinitial(psat) to the measured ETfinal = PRESSURE at work during the hydrodynamic stage!

6 OK but how about the detailed properties of QCD matter…?


History remark: Centrality dependence in EKRT was in fact not a problem !

Localizing the model for non-central collisions: psat=p0(√s, A, x,y)

EKRT prediction: Nch/Npart vs Npart flat or even slightly rising towards non-central A+A, seemed not agree with data…

[STAR, PRC79, 034909 (2009)]

7


[KJE, Kajantie, Tuominen, Phys.Lett. B497 (2001) 39]

History remark: Centrality dependence in EKRT was in fact not a problem !

Localizing the model for non-central collisions: psat=p0(√s, A, x,y)

EKRT prediction Nch/Npart vs Npart is flat or even slightly rising towards non-central A+A, did agree with data when the same optical Glauber model was used for Npart !

[STAR, PRC79, 034909 (2009)]

8

[This thorough STAR analysis revived also my interest in the more detailed EKRT studies discussed next]


[KJE, Kajantie, Tuominen, Phys.Lett. B497 (2001) 39]

9

2. Recent developments in EKRT - full NLO pQCD & improved minijet ET definition - new angle to saturation - viscous 2+1 D hydro - EbyE framework Basic idea: 1. Compute minijet (=gluons, pT= a few GeV) ET production in A+A, using NLO perturbative QCD + saturation conjecture for ET 2. Describe space-time evolution of QCD matter with viscous hydrodynamics initialized with fluctuating pQCD+saturation initial conditions, event by event 3. Compare with LHC & RHIC data for bulk (=low pT) observables, to - pin down QCD matter η/s(T) - test the initial state calculation and its predictive power - study the applicability region of viscous hydro

η/s(T) = ?

[Phys.Rev. C87 (2013) 044904] [Phys.Lett. B731 (2014) 126] [Phys.Rev. C93 (2016) 024907]

10

Minijet ET production in A+A and Δy from NLO pQCD

• s=(x,y) transverse position, Δy = unit rapidity window • TATA accounts for nuclear collision geometry • Collinear factorization, NLO pQCD in 22 and 2 3 parton scatterings:

• fi/A = spatially dependent nPDFs (see next page) • UV-renormalized |M|2 [Ellis,Sexton,Nucl.Phys. B269 (1986) 445, Paatelainen’s PhD thesis] • Ellis-Kunszt-Soper subtraction method [see KS, Phys.Rev. D46 (1992) 192; KJE, Tuominen, Phys.Rev. D63 (2001) 114006] with IR/CL safe measurement functions S2 & S3 to define the minijet ET in NLO

+… +… +…

11

- fip(x,Q2): free proton PDFs from CTEQ6M

- riA(x,Q2,s): spatially dependent NLO EPS09s nuclear PDF modifications from

[Helenius et al, JHEP 1207 (2012) 073], where the A-dependences of the EPS09 nPDF modification factors Ri

A(x,Q2) were converted into s-dependences via

Nuclear modifications are strongest near the center of a nucleus, and weaken towards the edge

Spatially dependent nPDFs

12

Measurement functions for computing minijet ET in NLO

• analogous to jet definition; Sn define - the minijet ET in Δy - what we mean by hard scattering (p0) - what is the min ET we may require in Δy • IR & CL safeness: S3 S2 at IR & CL limits • any β in [0,1] is OK leave β as a free parameter since the minijet ET is not a direct observable [Paatelainen, KJE, Holopainen, Tuominen, Phys. Rev. C87 (2013) 4, 044904] • with these Sn + given nPDFs, minijet NLO ET computation is well defined!

13

A new angle to saturation [Paatelainen,KJE,Holopainen,Tuominen, PRC87 (2013) 044904] instead of fusion of produced gluons, we conjecture saturation to happen when ET from 32, 42,… processes becomes of the same order as the ET from 22:

A

A

pT2 pT1 pT3 pT4

pT1 > pT2 > pT3 > pT4

14

Saturation criterion like in the original EKRT but now consistently for ET:

RA

Key observation: psat scales with TATA: This enables the EbyE framework for us…

[Paatelainen, KJE, Niemi, Tuominen, Phys.Lett. B731 (2014) 126]

here b= 0, 6.59, and 8.27 fm :

size of minijet production area

min(psat)=1 GeV

[Niemi, KJE, Paatelainen, Tuominen, Phys.Rev. C93 (2016) 014912]

Ksat from data

15

NLO EKRT EbyE framework • Nucleon positions in A: sample WS distribution • Around each nucleon, set a gluon cloud of transverse density σ= 0.43 fm from HERA data Overlap functions TA1(x,y) & TA2(x,y) psat=psat(TA1*TA2) (*) Local energy density at

• ”Pre-thermal” evolution from τsat= 1/psat(x,y) to 1/psat

min = 0.2 fm/c here done simply with 1 D Bjorken hydro at each (x,y) (we tested also free streaming, both OK) • Below psat

min = 1 GeV, connect smoothly to BC profile

run 2+1 D viscous hydro EbyE

[Niemi, KJE, Paatelainen, Phys.Rev. C93 (2016) 024907]

(*) Parametrization of psat(TA1TA2) vs (Ksat,β) is available for public use in Phys.Rev. C93 (2016) 024907

16 16

+ transient fluid-dynamics EoM for [Denicol,Niemi,Molnar,Rischke,PRD85(2012)114047] + s95p-PCE-v1 QCD EoS: Tchem= 175 MeV; Tfo=100 MeV [Huovinen,Petreczky,NPA837(2010)26]

Viscous Hydrodynamics [Niemi et al]

Neglect heat conductivity & bulk viscosity; Keep shear viscosity η; 2nd order dissipative relativistic hydrodyn.

Viscosity effects: - reduced flow-velocity gradients during the evolution - entropy increase from initial to final state - Non-equilibrium particle distributions on the freeze-out surface

Initial conditions in our EbyE case: - The computed EbyE-fluctuating energy densities Ɛ(x,y,τi=0.2 fm) - Initial vT= 0 - Initial πμν = 0

Centrality dependence of Nch comes out correctly; -- only one LHC-point (Ksat & β) is fitted, the rest is prediction

LHC RHIC

17 Our <initial transverse densities> [width of the gluon cloud!] are under control, but essentially no constraints for η/s(T) from this observable

Comparison with LHC and RHIC data

Map the possible T dependence of η/s(T) with these parametrizations, reproducing the measured v2 at LHC


18

[Niemi, KJE, Paatelainen, Phys.Rev. C93 (2016) 024907] Our centrality classification is under control

Entropy increases from initial to final state the more the QGP viscosity is!

We do not yet include dynamical fluctuations of psat, hence we do not (should not!) reproduce the highest-multiplicity tail

LHC RHIC

Centrality dependence of charged-hadron pT spectra ~OK

19 Our QCD matter EoS is under (sufficient) control but essentially no constraints for η/s(T) from here, either


Centrality dependence of 2,3-particle cumulant flow coefficients vn

Simultaneous LHC & RHIC analysis very important!

20

LHC RHIC

Constraints for eta/s(T): Small η/s(T) in the HRG seems favored

v2

v4

v3

LHC vns well reproduced by all these η/s(T)


21

Relative EbyE fluctuations of elliptic flow at LHC come out beautifully

Ɛ2=Ɛ2,2


22

Relative EbyE fluctuations of elliptic flow at LHC come out beautifully

No sensitivity to η/s(T) Constraint to the initial state Our initial states are in control

- To reproduce these measurements, need EbyE hydro: Initial spatial asymmetry correlates nonlinearly with final state momentum asymmetry!

Ɛ2=Ɛ2,2


23

Correlations of 2 Event-plane angles also OK, for centralities < 40-50%

Especially since P(δvn) constrain our ISs independently of η/s, these correlations give further constraints for η/s(T) and simultaneously test the validity of the EbyE viscous framework!


LHC

24

Even the correlations of 3(!) Event-plane angles similarly OK, for centralities < 40-50%

Remarkably, the same two η/s(T) parametrizations that explain the RHIC vn’s — the black and blue in the fig. — work best also at LHC! For these, also the viscous hydro seems best under control…

LHC


25

Symmetric 2-harmonic 4-particle (!) cumulants from ALICE

ALICE, arXiv:1604.07663 [nucl-ex] EKRT results from H.Niemi

The same two best η/s(T) parametrizations [0.2 & param1] work best also here!

26

Solid lines = with δf Dashed = without δf

Applicability region of viscous hydro: magnitude of δf corrections?

(decays not included in these figures)

Smallest hadronic viscosities (blue&black) work best: δf effects in vn remain small up to 40-50 % centralities


27

Applicability region of dissipative hydro: magnitude of δf corrections?

δf effects remain (mostly) small from central to semi-central collisions: constraints for eta/s in the applicability region of hydro!


Solid lines = with δf Dashed = without δf

28

3. Predictions for the 5.02 TeV Pb+Pb LHC run

[Phys.Rev. C93 (2016) 014912, arXiv:1511.04296 [hep-ph]]

blue . . . black 0-5% central: EKRT

29

3. Predictions for the 5.02 TeV Pb+Pb LHC run

vs. 5.02 TeV ALICE data [Phys.Rev.Lett. 116 (2016) 222302, arXiv:1512.06104 [nucl-ex]]


ALICE: 1943 +- 54 0-5% central: EKRT blue . . . black

30

Ratio of the flow coefficients vn{2} at 5.02 TeV and 2.76 TeV


EKRT prediction…

- Higher harmonics n > 2 more sensitive to η/s(T) - Further constraints for η/s(T)

31

Ratio of the flow coefficients vn{2} at 5.02 TeV and 2.76 TeV


EKRT prediction vs ALICE data [Phys.Rev.Lett. 116 (2016) 132302]

- Higher harmonics n > 2 more sensitive to η/s(T) - Further constraints for η/s(T)

32

Correlations of two EP angles for charged hadrons in 5.02 TeV Pb+Pb

Very similar to the 2 EP correlations at 2.76 TeV, i.e. similar constraining power for η/s(T) as at 2.76 TeV

EKRT 5.02 TeV prediction [Phys.Rev. C93 (2016) 014912, arXiv:1511.04296 [hep-ph]] vs. ATLAS 2.76 TeV data [Phys. Rev. C 90 (2014) 2, 024905]

33

Conclusions & outlook • NLO-improved pQCD+saturation+viscous hydro EbyE framework (EKRT model) - explains consistently the LHC and RHIC bulk observables in URHIC - has clear predictive power in cms energy, centrality, A - enables estimation of the QCD matter η/s(T) and its uncertainties • Now there starts to be enough orthogonal data constraints available from LHC and RHIC, for (i) pinning down the initial conditions, (ii) probing the validity of the framework and (iii) probing & determining the QCD matter η/s(T) – a simultaneous LHC and RHIC multiobservable analysis is required!

Our ”best” estimate currently for η/s(T) but this is not yet a true error band — statistical global analysis needed

• Similar η/s magnitudes also from - IP-glasma ISs: η/s = 0.12 (RHIC) … 0.2 (LHC) [Gale, Jeon, Schenke, Tribedy, Venugopalan, Phys. Rev. Lett. 110 (2013) 012302] - MCG/MC-KLN+VISHNU: 0.08 < const. η/s < 0.2 [Song, Bass,Heinz,Hirano, Shen, Phys. Rev. Lett. 106, 192301 (2011)]

34

Next in EKRT: • Include dynamical fluctuations of psat EKRT predictions in p+A collisions (?) • Develop a global analysis of these observables a statistical error band to η/s(T) • Improve the description of ”pre-thermal” evolution [Eff.Kin.Th./BAMPS] • Study also bulk viscosity effects, see e.g. Ryu et al, Phys. Rev. Lett. 115 (2015) 132301 Bernhard, et al., Phys.Rev. C94 (2016) 024907 • Need a ”MC-EKRT” event generator to study also y-dependent observables

• First attempt towards a statistical global analysis of data in [Bernhard,Moreland, Bass, Liu, Heinz, Phys.Rev. C94 (2016) 024907]

supports EKRT (and IP-glasma)-type initial states η/s(T) trend similar to EKRT indications of bulk viscosity(?)

35

Back up slides

36

bulk dN/dy ~OK


bulk <pT> ~OK

37

The vertical lines show where psat<1 GeV and where matching to BC profile is made

Average energy densities

Average initial eccentricities are btw eBC and eWN


eta/s=0.2

38


Parametrization of psat(Ksat,β) available:

39

Interestingly, the modest T-dependence of the hadronic viscosity obtained here in PCE is in fact not inconsistent with microscopic calculations in CE [e.g. Cernai, Kapusta, McLerran, PRL 97 (2006) 152303 ]


40 [Niemi, KJE, Paatelainen, Phys.Rev. C93 (2016) 024907]

41

[Niemi, KJE, Paatelainen, Phys.Rev. C93 (2016) 024907

Centrality dependence of 2,4-particle cumulant flow coefficients vn

42

EKRT prediction [Phys.Rev. C93 (2016) 014912, arXiv:1511.04296 [hep-ph]] vs. 5.02 TeV ALICE data [Phys.Rev.Lett. 116 (2016) 222302, arXiv:1512.06104 [nucl-ex]] , using ALICE’s Npart

[ALICE, PRL116 (2016) 222302]

data vs best EKRT fits data vs models

43

event plane angle Ψn = atan2(<sin nφ >/<cos nφ>)/n

F-components for each event:

vn = <cos(n(φ - Ψn ))>

high / low resolution

2-particle cumulant, not sensitive to Ψn[EP]

(no non-flow in our results)

3,4-particle cumulants

Participant plane angle

Exp’s:

44

Denicol, Koide, Rischke, Phys. Rev. Lett. 105, 162501 (2010) Denicol, Niemi, Molnár, Rischke, Phys. Rev. D85, 114047 (2012) Molnár, Niemi, Denicol, Rischke, Phys. Rev. D89, 074010 (2014)

EoM for shear-stress tensor from 14-moment approx to UR gas

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EbyE fluctuations in the EKRT pQCD+saturation ...crunch.ikp.physik.tu-darmstadt.de/erice/2016/sec/talks/thursday/... · EbyE fluctuations in the EKRT ... ultrarelativistic A+A collisions